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Article Cite This: Inorg. Chem. XXXX, XXX, XXX−XXX

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Partial and Complete Substitution of the 1,4-Benzenedicarboxylate Linker in UiO-66 with 1,4-Naphthalenedicarboxylate: Synthesis, Characterization, and H2‑Adsorption Properties Vera V. Butova,*,† Andriy P. Budnyk,† Konstantin M. Charykov,† Kristina S. Vetlitsyna-Novikova,† Aram L. Bugaev,† Alexander A. Guda,† Alessandro Damin,‡ Sachin M. Chavan,§ Sigurd Øien-Ødegaard,∥ Karl Petter Lillerud,∥ Alexander V. Soldatov,† and Carlo Lamberti*,†,⊥ Downloaded via IOWA STATE UNIV on January 9, 2019 at 19:13:17 (UTC). See https://pubs.acs.org/sharingguidelines for options on how to legitimately share published articles.

†

The Smart Materials Research Institute, Southern Federal University, Sladkova Street 178/24, Rostov-on-Don 344090, Russia Department of Chemistry, INSTM Reference Center and NIS Interdepartmental Center, and ⊥Department of Physics, INSTM Reference Center and CrisDi Interdepartmental Center, University of Turin, Via P. Giuria 1, Turin 10125, Italy § ProfMOF AS, Kirkegårdsveien 45, Kongsberg 3616, Norway ∥ Centre for Materials Science and Nanotechnology, Department of Chemistry, University of Oslo, Sem Saelands vei 26, Oslo 0315, Norway ‡

S Supporting Information *

ABSTRACT: We describe the synthesis and corresponding full characterization of the set of UiO-66 metal−organic frameworks (MOFs) with 1,4-benzenedicarboxylate (C6H4(COOH)2, hereafter H2BDC) and 1,4-naphthalenedicarboxylate (C10H6(COOH)2, hereafter H2NDC) mixed linkers with NDC contents of 0, 25, 50, and 100%. Their structural (powder X-ray diffraction, PXRD), adsorptive (N2, H2, and CO2), vibrational (IR/Raman), and thermal stability (thermogravimetric analysis, TGA) properties quantitatively correlate with the NDC content in the material. The UiO-66 phase topology is conserved at all relative fractions of BDC/NDC. The comparison between the synchrotron radiation PXRD and 77 K N2-adsorption isotherms obtained on the 50:50 BDC/NDC sample and on a mechanical mixture of the pure BDC and NDC samples univocally proves that in the mixed linkers of the MOFs the BDC and NDC linkers are shared in each MOF crystal, discarding the hypothesis of two independent phases, where each crystal contains only BDC or NDC linkers. The careful tuning of the NDC content opens a way for controlled alteration of the sorption properties of the resulting material as testified by the H2-adsorption experiments, showing that the relative ranking of the materials in H2 adsorption is different in different equilibrium-pressure ranges: at low pressures, 100NDC is the most efficient sample, while with increasing pressure, its relative performance progressively declines; at high pressures, the ranking follows the BDC content, reflecting the larger internal pore volume available in the MOFs with a higher fraction of smaller linkers. The H2-adsorption isotherms normalized by the sample Brunauer−Emmett−Teller specific surface area show, in the whole pressure range, that the surface-area-specific H2adsorption capabilities in UiO-66 MOFs increase progressively with increasing NDC content. Density functional theory calculations, using the hybrid B3LYP exchange correlation functional and quadruple-ζ with four polarization functions (QZ4P) basis set, show that the interaction of H2 with the H2NDC linker results in an adsorption energy larger by about 15% with respect to that calculated for adsorption on the H2BDC linker.

1. INTRODUCTION

possible SBUs and linkers leads to a great variety of MOF types. This wide field of molecular design is one of the reasons why MOFs are so popular nowadays. On the other hand, some families of MOFs have shown outstanding properties, making them attractive materials for many applications. For example, MOFs of the UiO-66 (named after the University of Oslo) series are known for their high thermal and chemical stability22−25 and exceptional tolerance to structural defects

Metal−organic frameworks (MOFs) are porous materials that have recently attracted much attention because of their tunable properties and therefore variety of applications.1−19 According to Yaghi and co-workers,20 there are two parts constructing the MOF structure: secondary building units (SBUs) and linkers. The geometry of the SBUs is defined by points of extension; they may contain one or several metal sites. The organic moleculeslinkersconnect SBUs into a 3D framework. The choice of SBUs and linkers determines the topology and symmetry of the resulting MOF.21 The endless number of © XXXX American Chemical Society

Received: November 7, 2018

A

DOI: 10.1021/acs.inorgchem.8b03087 Inorg. Chem. XXXX, XXX, XXX−XXX

Article

Inorganic Chemistry Table 1. Molar Ratios of Reagents for Synthesis of the Samples and Main Characteristic Parameters sample designationa

ZrCl4 (mol)

H2O (mol)

DMF (mol)

NDC (mol)

BDC (mol)

ab (Å)

SSAc (m2/g)

pore volume (cm3/g)

TGA peakd (°C)

0NDC (i.e., UiO-66) 25NDC 50NDC 100NDC

1 1 1 1

3 3 3 3

300 300 300 300

0 0.25 0.5 1

1 0.75 0.5 0

20.7582(4) 20.7948(3) 20.8285(5) 20.8538(8)

1061 936 731 488

0.415 0.366 0.249 0.164

535 525 500 480

a

Designation of samples reflects the fraction in molar percent of NDC in the NDC/BDC linker mixture used in the synthesis batch. bObtained from the Rietveld refinement of laboratory PXRD data. cObtained using the BET theory. dMaximum value of the first-derivative peak in the TGA plots.

(like missing linkers or SBUs).26,27 UiO-66 consists of Zr 6O 4 (OH) 4 SBUs connected to each other by 1,4benzenedicarboxylate (BDC) linkers.22−24,28 There are a few ways to affect its properties without alternating the structure: substitution of the BDC linker with another one possessing the same connecting functionalities;29−34 injection of a modulator to moderate the growth process;35−38 functionalization of the linkers by side functional groups;39−46 substitution in the SBU of the Zr(IV) metal cation with Hf(IV),47−49 Ce(IV),49−53 or Ti(IV)54−58 metal cation, cooperative cluster metalation, and ligand migration;59 etc. In our recent work,60 we replaced the BDC linker with the 1,4-naphthalenedicarboxylate (NDC) one and introduced benzoic acid into the reaction mixture as a modulator. We demonstrated that full substitution of BDC linkers with NDC analogues did not change the framework topology. The introduction of benzoic acid resulted in bigger crystallites of improved morphology. The modulator’s competitive linkage to SBUs led to a higher defect density (rising to almost 50%, depending on the quantity of the modulator) in the final material, characterized by increased specific surface area (SSA) and decreased thermal stability. The partial substitution of linkers or the use of two or more types of different linkers in the same synthesis provides an additional degree of freedom in the synthesis, which could significantly change the properties of the product. MOFs with mixed linkers attracted much attention in the last years61−64 because the resulting properties could not only result in simply linear sums of the pure-component properties but also have a synergetic effect in enhancing some specific properties. For example, Deng et al.62 reported on a MOF-5-type structure with a mixture of three linkers, BDC-NO2, BDC-(OC3H5)2, and BDC-(OC7H7)2, which exhibits up to 400% better uptake selectivity for carbon dioxide (CO2) over carbon monoxide (CO). The main problem in the mixed-linker MOF synthesis is obtaining a single-phase material with mixed linkers instead of a mixture of phases, each with a single linker. In the present work, we have investigated the set of compositions of UiO-66type MOFs with partial substitution of the BDC linker with the NDC one and proven that the BDC and NDC linkers are shared in each MOF crystal.

respective amounts of H2BDC and H2NDC were added under stirring to produce four samples with different molar ratio, as given in Table 1. After complete dissolution of the reagents has been reached, the reaction flask was sealed and placed in a preheated oven at 120 °C for 24 h. Crystallization was performed under static conditions. After cooling to room temperature, the resulting white solid was separated by centrifugation, washed twice with DMF and then once with THF, and dried at 60 °C in a conventional oven. 2.2. Characterization. The phase purity of the UiO samples was first determined by means of a laboratory-level powder X-ray diffraction (PXRD) D2 Phaser system (Bruker) operating with Cu Kα radiation (λ = 1.5418 Å). The 2θ = 5−60° data range was collected at step intervals of 0.02° with 0.1 s counting time per step. High-resolution diffraction patterns for profile analysis were then measured in 0.7 mm rotating glass capillaries at the Swiss−Norwegian Beamline (BM01B)65 of the European Synchrotron Radiation Facility (ESRF), Grenoble, France. Capillaries were filled and sealed in air. For each sample, 15 2D diffraction images were recorded with 5 s acquisition time by the CMOS-Dexela 2D detector. The same number of dark images was recorded for background subtraction. Both the wavelength λ = 0.51353(1) Å and the sample-to-detector distance were calibrated using LaB6 and silicon powder model samples from the National Institute of Standards and Technology. The adopted experimental setup allowed us to cover the 2θ = 2.0− 32.0° range. In the refinements, we used the shorter interval of 2θ = 4.5−31.0° range, which corresponds to the Q range from 0.30 to 8.51 Å−1 and to a d spacing ranging from 6.54 to 0.96 Å. Subsequent averaging and integration were carried out using the ESRF PyFAI software.66 Further profile analysis was done using Jana2006 software.67 The SSA and porosity were determined by the Brunauer− Emmett−Teller (BET) method68 from the N2-physisorption isotherm obtained (at −196 °C) on an ASAP 2020 (accelerated surface area and porosimetry) analyzer (Micromeritics). The sample was activated at 200 °C for 24 h in a dynamic vacuum before the measurement. The Barrett−Joyner−Halenda model69 was used for pore-size distribution. Raman spectra were recorded on a Renishaw Micro Raman instrument using 005% power of a 785 nm laser. Spectra were averaged on three different points, each measured with a 10× objective and 20 acquisitions. Fourier transform infrared (FTIR) spectra were recorded in transmission mode on a Vertex 70 (Bruker) spectrometer with a resolution of 2 cm−1. Determination of the linker vibrational modes was performed on samples prepared with the KBr pelleting technique. Conversely, measurements of the CO2 adsorption at room temperature were performed on the samples compacted in self-supporting pellets. Samples were fixed in a homemade quartz cell equipped with KBr windows, allowing for measurement in a controlled atmosphere. Prior to the measurement, samples were activated at 150 °C in a dynamical vacuum. About 100 mbar (75 mmHg) of high-purity CO2 was delivered into the cell. Transmission electron microscopy (TEM) was performed on a FEI Tecnai G2 Spirit TWIN transmission electron microscope operated at an accelerating voltage of 80 kV. Sampling was done by the dispersion of powders in absolute ethanol. The average particle size was calculated as an arithmetic mean of a set of 50−100 values. Thermogravimetric analysis (TGA) was performed on a Jupiter STA 449 F5 analyzer (Netzsch) with samples held in corundum pans

2. EXPERIMENTAL METHODS 2.1. Synthesis. The chemicals zirconium tetrachloride (ZrCl4), 1,4-benzenedicarboxylic acid [H2BDC, C6H4(CO2H)2], 1,4-naphthalenedicarboxylic acid [H2NDC, C10H6(CO2H)2], N,N-dimethylformamide [DMF; (CH3)2NC(O)H], and tetrahydrofuran (THF, C4H8O), all of analytical grade, were obtained from commercial suppliers and used as received. Deionized (DI) water (18 MΩ·cm) was obtained from a Milli-Q ultrapure water system. In a typical synthesis, ZrCl4 (0.250 g) was dissolved in 25 mL of DMF in a conical flask, and then 57.9 μL of DI water was added to reach a molar ratio of 1:3:300 ZrCl4/H2O/DMF. After that, B


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Inorganic Chemistry in a continuous nitrogen flow or in the flux of air with a heating rate of 10 °C/min. 2.3. Modeling. To estimate the binding energy between the H2 molecule and the organic linkers used in the UiO-66 synthesis investigated in this work, we calculated the geometries and energies for the different configurations of the H2 molecule adsorbed onto H2BDC and H2NDC linkers. The calculations were performed within the B3LYP density functional theory (DFT) level, as implemented in the ADF-2017 program package.70,71 The largest available quadruple-ζ with four polarization functions (QZ4P) basis set was used.72 Among others, the hybrid B3LYP73 exchange correlation functional with 20% exact Hartree−Fock exchange was used, which has recently shown its applicability to describe the H2−C sp2 interaction in the graphene sheet.74 D3 dispersion correction was applied to account for van der Waals interactions.75−77

3. RESULTS AND DISCUSSION 3.1. Structural Analysis and Morphology. The results of laboratory PXRD characterization of the samples (Figure S1) testified to the good degree of crystallinity and phase purity of the obtained samples, confirming the UiO-66-like phase in all cases. A detailed structural analysis has been made on the synchrotron PXRD data reported in Figure 1a in the 2θ range of 4.5−10.5°. For the full range of patterns, see Figure S2. Of interest is the intensity inversion of the couples of reflections (311)−(222) and (331)−(420) by moving from 0NDC to 100NDC. The refinement was made in the Jana2006 program67 (Figure S3). A spline background was subtracted from all of the patterns prior to the refinement to reduce the scattering contribution from the glass capillary. Three parameters of the pseudo-Voight function were used to describe the peak shape: GW, LX, and LY. The GW parameter was fixed to the value obtained for the LaB6 standard. For the studied samples, the refined values of the Gaussian crystallite size-broadening parameter (GP) were negligibly small; therefore, GP was set to 0. The GU value for the LaB6 refinement was negative and was also set to 0. The LX and LY parameters were used to calculate the crystal size and strain for the samples. In the first refinement [performed in the space group Fm3̅m (No. 225)] of the 0NDC sample (i.e., UiO-66), the occupancy of the Zr atom was fixed to 1, and all other occupancies were optimized. The resulting values were 0.93, 0.87, 0.84, 0.89, and 0.86 for the O1, C11, C12, and C13 atoms, respectively (see Figure 1b for atom labeling). Therefore, in the following refinements, all occupancies for the C atoms and the O1 atom of the linker were constrained to be equal. The O2 position was split into O2A and O2B with equal occupancies, reflecting μ3O and μ3OH atoms in the middle of the eight triangular sides of the Zr6O4(OH)4 SBU of UiO-66.23,24 The distances between different pairs of neighboring C atoms were also set to be equal (C11−C12 = C12−C13). As reported in our previous work on pure UiO-66-NDC,60 the contribution of C14 and C15 atoms to the electron density is relatively low because of their lower occupancy factor (taking into account the reduction due to symmetry) and the high anisotropic displacement due to the rotation of the linker. To refine all patterns with the same strategy, including the 25NDC and 50NDC ones, where the contribution of these atoms is even lower, we did not include the C14 and C15 atoms in the refinement procedure. This implies that the refined parameters for the 100NDC sample will be slightly different with respect to those published before, where all atoms of the NDC linker were refined.60

Figure 1. Part (a): Synchrotron radiation (λ = 0.51353) PXRD patterns of synthesized samples from bottom to top: 0NDC (blue), 25NDC (green), 50NDC (red) and 100NDC (brown), and mechanical mixture (orange) of 1:1 molar ratio of 0NDC and 100 NDC, superimposed on the 50NDC. Vertical dotted lines allow to appreciate the shift of the Bragg peaks (indexed on top) with increasing NDC content. Part (b): The dependence of the rotation angle of the average linkers (squares, left ordinate axis) and refined lattice parameter a (triangles, right ordinate axis) on the NDC content in the samples. Color designations as in part (a). The model in the bottom right corner of part (b) depicts connection of a linker with two SBU in the UiO-66-NDC structure. Blue polyhedra represent zirconium coordinated by oxygen ions, while the C atoms of the linker are represented by black spheres. Also reported are the labels used in the refinement to discriminate among crystallographic independent C and O atoms (atoms C14 and C15 are absent in BDC). The bent arrows indicate the C11−C12 rotational axis of the linker.

The C13 atom was moved from 96j to the less symmetric 192l site to allow rotation of the linker along the C11−C12 axis. We define as φ the rotation angle of the linkers, that is, the angle between the plane of the C atoms of the linker and the c−a direction (i.e., the dihedral angle between the O1− C11−C12 and C11−C12−C13 planes). Table 1 reports the main results of the Rietveld analysis on four samples. With increasing NDC content, the lattice parameter a rises from 20.7589(1) to 20.8556(5) Å. The progressive increase of the lattice constant is related to the stress created by extra benzene rings of the NDC linker in comparison with the standard BDC ligands. Of interest is also the progressive increase of the tilting angle φ of the linkers with increasing NDC content, needed to avoid the steric hindrance of adjacent NDC linkers.60 To check that the intermediate synthesis resulted in a single phase containing both linkers in the same crystals instead of two separate phases of pure MOFs with BDC or NDC linkers, we compare the PXRD pattern of the 50NDC sample with that C


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Inorganic Chemistry

Figure 2 reports, for the four samples with different NDC contents, representative TEM images showing that in all cases the crystals have an octahedral shape typical for the UiO-66 phase.60,78−80 3.2. Volumetric Analysis, H2-Adsorption Properties, and Related DFT Calculations. The N2-sorption isotherms (Figure S4) are all of type I (IUPAC classification),81 which is typical for microporous materials. For the sake of analysis, their adsorption branches are shown in the logarithmic scale in Figure 3a; this allows one to better appreciate the low-pressure region. The linear scale and whole pressure range for both the adsorption and desorption branches are presented in Figure S4a. As can be seen from Figure 3a, the tracks of isotherms in the low-pressure region deviate significantly on passing from that of the 0NDC sample to those of the samples with the NDC linker. In more detail, the isotherm of 0NDC exhibits three steps at relative pressures P/P0 near 4 × 10−6, 3 × 10−4, and 3 × 10−2, in good agreement with the previously reported data.82 All others have one step only, which progressively moves to lower P/P0 with increasing NDC content: 4 × 10−4, 2 × 10−5, and 5 × 10−6. A multistep adsorption isotherm was already observed in UiO-6682,83 and other MOFs.82,84,85 For ZIF-8 MOF, two possible explanations were proposed: (i) reorganization of adsorbed N2 molecules in the pores;84 (ii) an increase in the size of the pore windows after the threshold pressures were reached.85 For UiO-66, the phenomenon was explained in terms of the successive filling of the octahedral and tetrahedral cages82 or the gate-opening effect caused by pressure-induced linker tilt.83 The latter hypothesis could explain the absence of the multistep adsorption isotherm in

obtained on a mechanical mixture of 0NDC and 100NDC in a 1:1 molar ratio (red and orange curves, respectively, in Figures 1a and S2). Because of the significant difference in the lattice parameters between the 0NDC and 100NDC samples, the mechanical mixture resulted in an intrinsic broadening of the Bragg reflections, which progressively increases with increasing 2θ. This broadening is not observed in the 50NDC sample, implying that the linkers are mixed in each crystallite, resulting in a unique lattice parameter of intermediate value. We used the (333) reflection, which is well isolated, to quantify the phenomenon: the full width at half-maximum (fwhm) moves from 0.060° to 0.079° with an increase of 30% (Table 2). Using a higher index reflection, the difference would have been even larger. Table 2. Summary of the Rietveld Refinements of Synchrotron PXRD Dataa sample

cell parameter (Å)

fwhm(333) (deg)

φ (deg)

0NDC 25NDC 50NDC 100NDC MM

20.7589(1) 20.7892(2) 20.8301(2) 20.8556(5) 20.7979(3)

0.065 0.058 0.060 0.061 0.079

13 16 18 31 16

φ is the angle between the plane of the C atoms of the linker and the c−a direction (i.e., the dihedral angle between the O1−C11−C12 and C11−C12−C13 planes). MM = mechanical mixture of 0NDC and 100NDC (1:1 moles). The space group Fm3̅m (No. 225) was used in all cases.

a

Figure 2. TEM images of samples with increasing NDC content. D


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Inorganic Chemistry

Figure 3. (a) Logarithmic plot (in the low-pressure region) of N2 adsorption at 77 K on samples with different NDC contents. (b) Like part a for the 50NDC sample (red dots), compared with a mechanical mixture of 0NDC and 100NDC (1:1 in moles, purple dots) and with a linear combination (orange triangles) of the two isotherms collected on the MOFs synthesized with pure ligands (0NDC + 100NDC)/2 and reported in part a. (c) BET surface area (bar histogram, left ordinate axis) and micropore volume (colored dots, right ordinate axis) of samples with different NDC contents.

Figure 4. (a) H2-adsorption (solid circles) and H2-desorption (open circles) isotherms collected at 77 K for samples with different NDC contents. (b) Like part a, renormalized by the BET SSA of the different MOFs (Table 1). A similar result is obtained when normalization is made with the pore volume value (Figure S5).

Table 3. Relative Ranking of Samples with Different NDC Contents in the Amount of H2 Adsorption in Different Pressure Ranges P(H2) (mmHg) 1st material 2nd material 3rd material 4th material

30

100NDC 0NDC 50NDC 25NDC





0NDC and 100NDC surface areas (774 m2/g) and that differs significantly from that of the 50NDC sample (732 m2/g). The SSA values were calculated by the BET method68 and presented with respect to the NDC content in Figure 3c and Table 1. SSA (micropore volume) decreases from 1061 m2/g (0.415 cm3/g) to 488 m2/g (0.164 cm3/g) with an increase of the NDC fraction, which is expected because of occupation of the pore’s space by the more bulky naphthalene rings. Finally, in the N2 isotherms, we have observed a small hysteresis loop for the samples 50NDC and 100NDC (Figure S4a). In this regard, it is worth mentioning that similar hysteresis loops have been observed by Liu et al.86 in HKUST-1.87,88 The authors provided evidence for the formation of mesopores due to partial replacement of the BTC linkers by a second ligand (benzoic acid). We believe that a similar effect is also taking place in the present case of the mixed ligand UiO-66. This is a relevant point because the presence of mesopores in UiO-66

samples containing NDC linkers because they are already tilted in their equilibrium position.60 Moreover, we used the slope of the N2 isotherms as a fingerprint to prove that the NDC and BDC linkers mix into a single phase, confirming the analogous comparison done with PXRD experiments (Figure 1a and Table 1). To this aim, we have compared the isotherms of a mechanical mixture of 0NDC and 100NDC samples with that of the 50NDC sample (Figure 3b in the low-pressure range; see Figure S4b for the whole range). The measured isotherm of the mechanical mixture (purple curve) is in good agreement with the mathematical average of the 0NDC and 100NDC isotherms (orange curves), while the 50NDC one differs from it and could not be obtained as a simple mathematic combination of the 0NDC and 100NDC isotherms in both low and high P/P0 ranges. The BET SSA of the mechanical mixture is 771 m2/g, a value that is in a good agreement with the average mean of the E


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Inorganic Chemistry can overcome the limitations of UiO-66 for many applications because of the restricted size of their micropores. The development of synthesis procedures aimed to create mesoporosity in MOFs is a highly investigated topic86,89−92 because the presence of mesopores, resulting in hierarchical structures, represents a significant improvement of the MOF diffusion properties, especially when the mesoporosity can be controlled at will during synthesis. H2-adsorption isotherms are presented in Figure 4a. The H2 uptake at high pressures decreases with an increase of the NDC content, in good agreement with the BET SSA values. This effect, however, does not hold for the whole pressure range; the relative ranking of the four materials changes with pressure, as reported in Table 3. Indeed, up to 5 mmHg, the H2 uptake is larger for the 100NDC sample, and then with increasing pressure, the relative ranking of this material starts to progressively decline. This effect can be explained in terms of a slightly more efficient interaction between the H2 molecule and the naphthalene rings, with respect to the benzene one and by the fact that there are two rings available for adsorption in the case of the NDC linker. There is a compromise between the presence of the NDC linker and the total surface area available in determining the ranking scale of the four materials: at low pressure, the former prevails, and at higher pressure, the latter dominates. At pressures larger than 30 mmHg, the ranking is uniquely driven by the SSA of the material. If we normalize the H2-adsorption isotherms of Figure 4a by the BET SSA value, we obtain the curves reported in Figure 4b, which clearly shows that the H2 adsorption per unit of internal surface area is significantly higher for the 100NDC sample than for the 0NDC one, in the whole pressure range. A comparable result is obtained when normalization is made with the pore volume value, as reported in Figure S5. Finally, we have observed very small hysteresis loops in samples 25NDC and 50NDC and more consistent in the 100NDC sample. The phenomenon is attributed to the retention of H2 molecules by the naphthalene ring system.93,94 To support the experimental findings reported in Figure 4 and Table 3, we performed DFT calculations (see section 2.3) on H2 adsorption for both the H2BDC and H2NDC linkers. The optimized geometries are reported in Figure 5, while relevant quantitative geometrical and energetical values are listed in Table 4. To simulate, in the first approximation, the constraints imposed by the insertion of the linkers inside the MOF framework, the positions of the four O atoms of the carboxylate units have been fixed to the crystallographic positions obtained in the XRD refinements performed on UiO6624 and on UiO-66-NDC60 for the H2BDC and H2NDC linkers, respectively. On the H2BDC linker, the side-on geometry (Figure 5a) is slightly preferred with respect to the end-on one (Figure 5b) by 0.291 kJ/mol and results in an adsorption distance of dH2−C6 = 2.97 Å, measured from the center of mass of the H2 molecule and the plane of the six C atoms. The adsorption angle is slightly tilted by 5° with respect of the C-atom plane (Figure 5a). For the end-on configuration, the optimized geometry differs by more than 30° from the starting one. Adsorption of the H2 molecule on the H2NDC linker can occur either on the ring connected to the carboxylate units (ring R1, Figure 5c,e, side- and end-on geometries, respectively) or on the adjacent one (ring R2, Figure 5d,f, side- and end-on geometries, respectively). The DFT calculations show that for both side- and end-on configurations the presence of two adjacent sp2-hybridized C

Figure 5. Optimized geometries for the adsorption of H2 on the linkers: (a) side-on starting geometry on the H2BDC linker; (b) endon starting geometry on the H2BDC linker; (c) side-on starting geometry on the H2NDC linker, ring R1; (d) side-on starting geometry on the H2NDC linker, ring R2; (e) end-on starting geometry on the H2NDC linker, ring R1; (f) end-on starting geometry on the H2NDC linker, ring R2.

rings slightly enhances the interaction energy of H2 with the π orbitals of the aromatic ring. This holds for adsorptions on both the R1 and R2 rings of the H2NDC linker (Table 3). Adsorption on the R2 ring results in two similarly optimized adducts (both structural and energetic grounds), while adsorption on R1 clearly favors the side-on geometry with an adsorption energy of 4.656 kJ/mol, an adsorption distance of dH2−C6 = 2.95 Å, a significantly tilted angle of 27° (Table 3 and Figure 5c). This geometry represents the more stable one for the H2 molecule among the investigated ones and is energetically more favored than the best one for the H2BDC linker by 15%. This computational study explains the experimental evidence that, at low equilibrium pressure, H2 adsorption is more efficient in the 100NDC sample and that, F


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Inorganic Chemistry Table 4. Summary of the DFT Study of H2 Adsorbed on H2BDC and H2NDCa linker

ads site

ads geometry

ΔE (meV)

ΔE (kJ/mol)

ΔE/E (%)

dH2−C6 (Å)

α (deg)

H2BDC H2BDC H2NDC H2NDC H2NDC H2NDC

R1 R1 R1 R1 R2 R2

end-on side-on end-on side-on end-on side-on

44.45 41.44 46.86 48.25 47.35 47.68

4.289 3.998 4.521 4.656 4.568 4.600

0 0 +5.4 +15.1 +6.5 +7.3

3.03 2.97 3.00 2.95 3.04 3.02

69 5 68 27 69 63

a

R1 is the benzene ring connected via the carboxylates units to the MOF framework, and R2 is the adjacent one present in H2NDC only. Both endand side-on adsorption geometries were tried. Adsorption energies are reported in both millielectronvolts and kilojoules per mole. ΔE/E represents the percentage of increased adsorption energy observed for H2 adsorption on H2NDC with respect to that obtained for adsorption on H2BDC with the same geometry. dH2−C6 is the distance between the center of mass of the H2 molecule and the plane of the adsorption ring. α is the angle between the H2 molecule axis and the plane of the adsorption ring: in the starting configuration, α = 0° and 90° for the side- and end-on configurations, respectively.

only at higher pressure, the adsorption ranking progressively favors samples with a higher internal available volume (Table 3). 3.3. Vibrational Properties: Framework Modes and CO2 Adsorption. Vibrational spectroscopies represent a set of powerful characterization tools in understanding the MOF structure, composition, defectivity, reactivity, and surface properties.23,32,38,88,95−113 The vibrational features of the whole set of samples is reported in parts a and b of Figure 6

Table 5. Summary of the Main Linker-Specific Vibrational Modes Observed in the Raman (Figure 6a) and IR (Figure 6b) Spectra Measured in This Work and Corresponding Assignments from the Literature, When Available (L n-s = Linker Nonspecific)

Figure 6. Vibrational study of samples with different NDC contents reported in the linkers f ingerprint region. In both parts, the spectra are vertically shifted for clarity (increasing the NDC content from top to bottom). (a) Raman spectra obtained after subtraction of the fluorescence background. (b) FTIR spectra of samples diluted in KBr, the bare spectrum of which is reported as a gray curve in the bottom. Vertical dashed guidelines refer to the modes that are specific for BDC (blue) or NDC (brown) linkers. Linker-unspecific IR bands at 667 and 1578 cm−1 are highlighted with back vertical guidelines in part b. See Table 5 for the exact wavenumber of each mode and for the corresponding assignment.

for Raman and IR, respectively. From a structural point of view, both BDC and NDC have the same functional groups, implying a very similar vibrational profile. However, similar modes will occur at slightly different wavenumbers in the two linkers, allowing easy recognition of their spectral signature. The more relevant vibrational modes in both the Raman and IR spectra are listed in Table 5 (top and bottom parts, respectively), together with the corresponding assignment from the literature,38,114,115 when available. The linker-specific bands are highlighted by vertical guidelines of blue and brown

ν (cm−1)

linker

634 669 781 863 1146

BDC NDC NDC BDC BDC

1359 1431 1438

NDC NDC BDC

1451

BDC

1520 1586 1618

NDC NDC BDC

667 748 791 1267

L n-s NDC BDC NDC

1367 1398

NDC BDC

1415

NDC

1460 1506 1516 1578 1657 3672

NDC BDC NDC L n-s NDC L n-s

3668

L n-s

assignment Raman Spectra benzene ring deformation in terephthalates C−H out-of-plane symmetric bending C−H out-of-plane asymmetric bending

ref 38 115 115

terephthalate ring breathing + benzoate ring deformation C−C stretching + ring deformation C−C stretching + C−H bending OCO symmetric stretching in carboxylate in-phase OCO symmetric stretching in carboxylate in-phase in-plane ring deformation CC stretching of aromatic rings CC stretching of aromatic rings IR Spectra

38

C−H wagging in-phase C−H wagging in-phase C−H bending out-of-phase and C−C stretching C−C stretching and C−H bending OCO symmetric stretching in carboxylate out-of-phase OCO symmetric stretching in carboxylate out-of-phase C−C stretching and C−H bending

114 this work 114

CC stretching OCO asymmetric stretching in carboxylate

114 38

O−H stretching mode of unperturbed SBU μ3OH O−H stretching mode of SBU μ3OH perturbed by NDC

Figure 7a−d Figure 7b−d

114 114 38 38 115 114 38

114 38 this work 114

color for the BDC and NDC linkers, respectively. Following the guidelines, when the NDC contents of the MOFs (from top to bottom in Figure 6) is increased, the increase of the NDC-specific bands and decrease of the BDC-specific ones are evident. This trend is, however, not perfectly linear with the G


Article

Inorganic Chemistry

Figure 7. (a) FTIR spectra of CO2 adsorption (at room temperature) on the 0NDC sample at different PCO2 values (0, 0.3, 1, 3, 6, and 60 mbar). The left (3700−3600 cm−1) and right (2400−2250 cm−1) panels refer to the O−H stretching and CO2 ν3 stretching regions, respectively. (b−d) Like part a for the 25NDC, 50NDC, and 100NDC MOFs, respectively. (e) Graphical representation of the inorganic Zr6(OH)4O4 SBU with two adjacent BDC linkers. The structure was taken from the single-crystal XRD refinement of 0NDC (UiO-66; φ ∼ 0°).24 (f) Like part e with two adjacent NDC linkers. The structure was taken from the PXRD refinement of 100NDC (UiO-66-NDC; φ = 30°).60

investigating the potentialities of MOFs as porous materials for CO2 capture.121−133 In this work, IR spectroscopy was used to follow CO2 adsorption at room temperature as a function of increasing CO2 equilibrium pressure (PCO2) on the samples with different NDC contents (Figure 7a−d; for each part, the left panel reports the O−H stretching region, while the right one reports the ν3 stretching mode of the CO2 molecule). In the gas phase, CO2 is a linear triatomic molecule that exhibits three vibrational modes, usually defined as ν1 (symmetric OC O stretching frequency, Raman active at 1388.3 cm−1), ν2 (doubly degenerate bending vibration, IR active at 667.3 cm−1), and ν3 (asymmetric OCO stretching frequency, IR active at 2349.3 cm−1).134 In our case, only the ν3 region can be investigated because both ν1 (IR active upon molecular adsorption) and ν2 are obscured by strong framework modes of the UiO-66 framework. Of interest is the O−H stretching region of the activated MOFs before CO2 dosage: lowest curve in the left panels of parts a−d of Figure 7. The 0NDC sample exhibits the wellknown sharp band at 3672 cm−1 due to the μ3OH stretching mode of the unperturbed inorganic Zr6(OH)4O4 SBU of UiO66.23,32,135 This band remains visible in all samples, but starting from 25NDC, a new component develops at 3668 cm−1, first as a shoulder of the former band and then as the main component in that region (sample 100NDC). We attribute this new band at the μ3OH stretching mode of the inorganic Zr6(OH)4O4 SBU perturbed by the second ring of the NDC linker. Indeed, while the C−H terminals of the BDC linkers are far away from the μ3OH groups of the SBU in UiO-66 (Figure 7e), they became much closer in the case for the NDC linkers. This allows the formation of a weak O···H bond between the H atom of the C−H group and the O atom of the μ3OH groups (Figure 7f), with a consequent small awakening of the O−H bond reflected by a red shift of its stretching frequency by 4 cm−1. Coming to CO2 adsorption, two ν3 bands are observed at 2338 and 2327 cm−1 (±1 cm−1 in the four samples). The bands are red-shifted with respect to the CO2 gas phase by 11

nominal NDC molar fraction, probably reflecting a slightly different incorporation fraction from the synthesis batch into the solid phase. The minor number of Raman-active modes makes the discrimination between the BDC and NDC bands more straightforward in the Raman spectra. IR bands are more convoluted, although the differences between the two extreme syntheses are also well-defined. For the UiO-66 sample (0NDC), the most intense Raman band at 1618 cm−1 is attributed to the CC aromatic stretch in the phase of the BDC linker, while the vibrational manifestation of the aromatic-ring in-plane bending is located at 634 cm−1 (Figure 6a).38 These modes move to 1585 and 668 cm−1 in the Raman spectra of the 100NDC sample. The doublet peaking at 1452 and 1438 cm−1 is due to in-phase OCO symmetric stretching of the carboxylate group in the BDC linker,38 which is replaced by a wide band peaking around 1431 cm−1 for the 100NDC sample, although this broad band is also visible at the foot of the doublet for all samples containing NDC. To conclude with a description of the spectral profile of the 0NDC sample, we mention that the peak at 1146 cm−1 is due C−C symmetric ring breathing,38 while that at 863 cm−1 is assigned to OH bending with some contribution from C−C symmetric breathing.116 Instead, the 100NDC sample also contains bands at 1520 and 1359 cm−1 related to in-plane ring deformations and another one at 781 cm−1,114,115 ascribed to out-of-plane asymmetric C−H bending.115 The FTIR spectra in Figure 6b show a complementary picture with a similar trend of the band appearance with respect to changing fractions of BDC/NDC linkers. The major features are the out-of-phase OCO symmetric stretching in carboxylate that occurs at 1398 cm−1 in 0NDC,38 that moves to 1415 cm−1 in 100NDC; the in phase C−H wagging mode at 748 cm−1 that shifts to 790 cm−1 moving from 0NDC to 100NDC and a band at 1657 cm−1, visible only when the NDC linker is present. The urgent problem of reducing anthropogenic CO2 emissions117−120 has encouraged an impressive effort in H


Article

Inorganic Chemistry and 22 cm−1, respectively. The presence of two red-shifted components in the ν3 mode of CO2 adsorbed inside MOFs is quite common and already observed, e.g., for CPO-27-Ni (2341 and 2329 cm−1),98 HKUST-1 (2342 and 2333 cm−1),96 and MIL-100(Fe) (2344 and 2334 cm−1).103 This differs from that observed upon adsorption of CO2 inside metal-alkali zeolites, where a single blue-shifted band was observed.136,137 For a full quantitative understanding of the observed ν3 frequencies, a DFT study is needed because the shift of the ν3 mode cannot simply be correlated to the adsorption enthalpy of CO2 on the specific site but is a complex combination of electron donation through the O atom and electron acceptance through the C atom of the CO 2 molecule;138 such an investigation is, however, beyond the scope of the present work. Of interest is the fact that μ3OH bands (both 3672 and 3668 cm−1 components) are not affected by CO2 adsorption, in none of the samples, meaning that CO2 is not interacting with such groups at the temperature and pressures investigated in this work. Indeed, the broad absorption centered in the 3636− 3632 cm−1 interval is not due to perturbed OH groups139,140 but is the combination of ν1 and ν3 modes of adsorbed CO2.96,98 The very weak band around 2275 cm−1 is due to the natural 13C abundance in CO2.96,98 Of relevance is also the absence of any band in the 2450−2380 cm−1. Bands in this region were observed upon adsorption of CO2 on exposed Cu2+ in HKUST-1 (2400 cm−1)140 and on Ni2+ in CPO-27-Ni (2408 cm−1)98 and alkali-metal exchanged M-ZSM-5 zeolites (on Li+, Na+, K+, and Cs+ at 2427, 2416, 2408, and 2400 cm−1, respectively)137 and attributed to a combination of ν3 with a metal-framework vibration. The absence of such a band in the spectra reported in Figure 7a−d evidences the absence of the coordination vacancy on the Zr4+ centers in UiO-66 frameworks. Because of the relatively low extinction coefficient of such combination bands, we do not exclude a minor presence of defective sites in studied samples. 3.4. Thermal Stability. TGA curves of all samples (Figure 8a) revealed a first weight loss at the temperature below 100 °C, which is attributed to H2O molecule evacuation from the pores. The TGA curve of the sample 0NDC has an additional small weight loss at 300 °C associated with DMF evacuation.23,27,36,37 The temperature of decomposition of the obtained samples decreases with an increase of the NDC content from 530 °C (0NDC) to 480 °C (100NDC), as better

evidenced in the first-derivative curves reported in Figure 8b (see Tables 1 and S1 for quantitative values).

4. CONCLUSIONS We have successfully synthesized the set of UiO-66 MOFs with BDC/NDC mixed linkers: samples 0NDC (i.e., UiO-66), 25NDC, 50NDC, and 100NDC (i.e., UiO-66-NDC). Their structural, absorptive, and vibrational properties quantitatively correlate with the NDC content in the material. It is important to notice that the UiO-66 phase topology is preserved at all relative fractions of BDC/NDC. The comparison between synchrotron radiation PXRD and 77 K N2-adsorption isotherms obtained on the 50NDC sample and on a mechanical mixture of 0NDC and 100NDC samples univocally proves that in sample 50NDC the BDC and NDC linkers are shared in each MOF crystal and discard the hypothesis of two independent phases, where each crystal contains only BDC or NDC linkers. The careful tuning of the NDC content opens a way for controlled alteration of the sorption properties of the resulting material, as testified by H2-adsorption experiments showing that the relative rankings of the materials in the H2 adsorption are different in different equilibrium pressure ranges: at low pressures, 100NDC is the most efficient sample, while with increasing pressure its relative performance progressively declines; at high pressures, the ranking follows the BDC content, reflecting the larger internal pore volume available in the MOFs with a higher fraction of smaller linkers. The H2-adsorption isotherms normalized by the sample BET SSA show, in the whole pressure range, that the surface-areaspecified H2-adsorption capabilities in UiO-66 MOFs increase progressively with increasing NDC content. These results are supported by the DFT calculations. Finally, the presence of a significant hysteresis loop in the N2-adsorption isotherm for the 50:50 BDC/NDC sample indicates the presence of mesopores, implying that hierarchical UiO-66 MOFs can be obtained by properly toning the linker ratio, with obvious improvement of the MOF diffusion properties.

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ASSOCIATED CONTENT

S Supporting Information *

The Supporting Information is available free of charge on the ACS Publications website at DOI: 10.1021/acs.inorgchem.8b03087.

■

Laboratory PXRD patterns for all samples, synchrotron PXRD patterns for all samples (and for the mechanical mixture of a 1:1 molar ratio of 0NDC and 100NDC) in the full collected 2θ range, comparison between the observed and calculated (from Rietveld refinement) and difference PXRD profiles for the samples, N2-adsorptiopn isotherms collected for all samples (and for the mechanical mixture of a 1:1 molar ratio of 0NDC and 100NDC) and reported in the whole pressure interval (linear scale), H2-adsorption isotherms collected for samples normalized by the pore-volume values of the different MOFs, and quantitative details on the TGA experiments (PDF)

AUTHOR INFORMATION

Corresponding Authors

*E-mail: [email protected]. *E-mail: [email protected].

Figure 8. TGA thermograms (a) and first-derivative curves (b) of samples with different NDC contents. I


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Aram L. Bugaev: 0000-0001-8273-2560 Sachin M. Chavan: 0000-0002-9947-1018 Sigurd Øien-Ødegaard: 0000-0001-7913-4199 Carlo Lamberti: 0000-0001-8004-2312 Notes

The authors declare no competing financial interest.

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ACKNOWLEDGMENTS We are indebted to Silvia Bordiga for fruitful discussion. The Open Access Raman Laboratory at the NIS Interdepartmental Center of the Turin University is gratefully acknowledged. V.V.B. thanks Boris Bouchevreau for his support during her time at the Chemistry Department of the Oslo University. V.V.B., A.P.B., K.M.C., K.S.V.-N., A.L.B., A.A.G., A.V.S., and C.L. are thankful the support of the Mega-Grant of Ministry of Education and Science of the Russian Federation (Grant 14.Y26.31.0001). A.V.S., V.V.B., and K.S.V.-N. are thankful for the financial support of Russian Foundation for Basic Research to Research Project 18-29-04053. We are indebted to Vladimir Dmitriev, Herman Emerich, Wouter van Beek, and Michela Brunelli for their friendly and competent support during the experiment performed at the BM01B (now moved to BM31) beamline of the ESRF.

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